Brief Description of the Drawings
FIG. 1 drawing of a prior art ring laser gyro using two gradient index rods to extract light from the counterpropagating laser beams of the ring laser.
FIG. 2 is a view, partly in section, showing two gradient index rods positioned to intercept light from the counter-propagating ring laser beams and to deliver such light through a symmetric single mode fiber-optic path to single mode fiber optic coupler and thence a three light detector.
FIG. 3, is a schematic diagram of a typical single mode fiber optical coupler connected as in this invention.
Description of the Preferred Embodiment
FIG. 1 shows a typical three-branched ring laser gyro according to U.S. Pat. No. 4,444,502. A ring laser body 10 has therein a conduit for supporting a ring laser path 12. The body is preferably rigid, and it is usually of glass-ceramic material. The body 10 is typically supported for angular mechanical dithering upon a set of flexure springs 14. The mirrors 16, 18 and 20 define the optical path of the gyro, and the mirror 20 is shown partly transparent so that a portion of each of the counterpropagating beams is directed to a separate gradient index rod 22 or 26.
The rods 22 and 26 are preferably identical, and they are attached into the mirror block 20 by an optically transparent adhesive which minimizes optical reflections at the interface. The rods 22 and 26 focus their received light onto their axis and hence onto the axis of the attached single mode fibers 24 and 28. The single mode fibers 24 and 28 can be attached onto the end of the rods 22 and 26 with an optically transparent adhesive.
The lengths of the single mode fibers 24 and 28 are preferably substantially equal, and they are connected to two of the input single mode fibers of the single mode fiber optical coupler 40. The output optical single mode fibers connect the coupler 40 to the three light sensors 42, 44, and 46.
The coupler is called a 3.times.3 single mode fiber optical coupler, and it preferably is an equal energy coupler wherein all of the incoming light is coupled from each single mode fiber into the other single mode fibers. A coupler which splits the energy equally in one labeled T-7270 manufactured by the Electro-Optical Products Division of the ITT Corporation at 7635 Plantation Road, Roanoke, Va. 24019. The theory for such couplers is described in:
"Optical Fiber Interferometers with 3.times.3 Directional Couplers Analysis" by S. K. Sheem, Journal of Applied, Physics, Volume 52, page 3865, (1981).
"Optical Techniques to Solve the Signal Fading Problem in Fiber Interferometers" by S. K. Sheem, T. G. Gialorenzi, and K. P. Koo, Applied Physics, Volume 21, page 689 (1982).
The apparatus of the invention operates without exact equal energy distribution, and the phases between the signals are altered by a change in energy distribution. Equal energy distribution and a three phase signal are preferred.
Typical equal energy distribution couplers have the three mode fibers in physical contact, perhaps side by side or intertwined so that light from each single mode fiber mixes with the light introduced from the other single mode fibers. The fibers within an equal energy coupler are positioned so that their cross section would show them positioned in a touching equilateral triangle configuration. This would be the geometry regardless of whether the fibers were side by side or intertwined.
Unequal attentuation of the different fibers within the coupler would also cause unequal energy distribution and unpredictable phase shift.
Although single mode fibers are specified herein, the invention functions with reduced efficiency when the fibers 24 and 28 are multimode fibers and the coupler 40 is still made from single mode fibers.
A 2.times.2 coupler could not be used efficiently because, although a single phase signal would be produced, there would be no indication of the polarity of the sensed rotation.
It would be difficult to use any other n.times.n coupler than a 3.times.3 coupler because the distance between centers of the fibers in the coupler would not all be equal, there would be unequal energy distribution, and it would produce unpredictable phase shifts. It is, however, intended that this patent application shall include the use of n.times.n and n.times.m couplers.
It is the inventors' intention that this invention should also include the basic concept of producing a substantially balanced set of three phase signals at all of the difference frequencies between individual pairs of light beams connected to the input ports of an equal energy distribution 3.times.3 coupler.
With the three output ports of the 3.times.3 coupler illuminating three photosensors, a three phase signal is produced between the electrical output terminals of the three photosensors at each of the difference frequencies between light sources connected to the coupler's input ports.
With only two light beams, of different optical frequencies, connected to only two of the input ports, a substantially balanced three phase signal is produced, at the photosensors, having a frequency equal to the difference frequency between the two light beams.
With three light beams, of different optical frequencies, connected to three input ports, three substantially balanced three phase signals are produced, at the photosensors, having three frequencies equal to the difference frequencies between the three light beams.
Although the invention has been described in detail above, it is not intended that the invention shall be limited by that description, but only by the description taken together with the appended claims.